超晶格
凝聚态物理
杰纳斯
材料科学
石墨烯纳米带
热电效应
丝带
半导体
声子
单层
光电子学
纳米技术
石墨烯
物理
热力学
复合材料
作者
Dan Han,Man Wang,Xiaoheng Yang,Mu Du,Lin Cheng,Xinyu Wang
标识
DOI:10.1016/j.jallcom.2022.163850
摘要
Transition metal dichalcogenide monolayers have shown enormous potential in thermoelectric application in recent years. We now focus on the thermoelectric properties of WS 2 -WSe 2 nanoribbons with superlattice (SL) and Janus (JA) structures using first-principles calculations. The WS 2 , WSe 2 , SL, and JA nanoribbons with the ribbon width from 5 to 7 have high structural stabilities. All nanoribbon electronic structures are semiconductors and the ribbon width will modify bandgaps. It can be also observed that WS 2 , SL, and JA nanoribbons with a ribbon width of 5 have the largest carrier mobilities (up to ~500–1400 cm 2 V −1 s −1 ) and relaxation times (up to ~400–600 fs). We further calculate the electronic transport coefficients and discover that the SL and JA nanoribbons with a ribbon width of 5 exhibit the largest power factors as high as ~80 mW m −1 K −2 . Afterwards, the minimum lattice thermal conductivities of SL and JA nanoribbons are 0.53 W m −1 K −1 and 0.61 W m −1 K −1 , which are suppressed owing to the declining phonon group velocity and phonon lifetime. The maximum ZT values of SL and JA nanoribbons can reach 5.47 and 4.13. This investigation provides a solid evidence for the application of WS 2 -WSe 2 nanoribbons as promising thermoelectric materials. • All WS 2 -WSe 2 nanoribbons have stable state and semiconducting properties. • Superlattice and Janus nanoribbons have large carrier mobilities. • The smallest k ph of superlattice and Janus nanoribbons are 0.53 and 0.61 W m −1 K −1 . • The high ZT of 5.47 and 4.13 for superlattice and Janus nanoribbons are obtained.
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